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Question: The temperature at which the speed of sound in air becomes double of its value at \({0^ \circ }C\) i...

The temperature at which the speed of sound in air becomes double of its value at 0C{0^ \circ }C is
a) 273K273K
b) 546K546K
c) 1092K1092K
d) 0K0K

Explanation

Solution

The speed of sound in a solid depends on the Young’s modulus of the medium and also speed of sound is inversely proportional to the root of molecular mass. Speed of sound depends on the density of the material, and the density depends on the temperature.

Complete step by step answer:
In an ideal gas, the equation speed of the sound in air is given by

v=γRTMv = \sqrt {\dfrac{{\gamma RT}}{M}} ……………...( 1)

In this formula, γ\gamma is the adiabatic index at room temperature (value depends on material to material) which is constant for air, R = 8.31 J/mol KR{\text{ }} = {\text{ }}8.31{\text{ }}J/mol{\text{ }} \cdot K is the gas constant, TT is the absolute temperature in kelvins, and MM is the molecular mass.
Velocity of sound is given by

vTv \propto \sqrt T .........................(2)

γ,R\gamma ,R, and MM are constant,

According to given statement,
Speed of sound in air become double,

say v1{v_1} =2×vs2 \times {v_s} at 0C{0^ \circ }C
v1v2=T1T2\dfrac{{{v_1}}}{{{v_2}}} = \sqrt {\dfrac{{{T_1}}}{{{T_2}}}} ……………...(3)

Now, v1v0c=2\dfrac{{{v_1}}}{{{v_{{0^ \circ }c}}}} = 2 (Speed of sound become double)
Temperature conversion, 0C{0^ \circ }C to Kelvin (0C+273.15)=273.15K({0^ \circ }C + 273.15) = 273.15K

2=T10+273.152 = \sqrt {\dfrac{{{T_1}}}{{{0^ \circ } + 273.15}}} ………………...(4)
(2)2=T1273.15{(2)^2} = \dfrac{{{T_1}}}{{273.15}}
4=T1273.154 = \dfrac{{{T_1}}}{{273.15}}

Now Solving above equation we get,

41=T1273.15K\dfrac{4}{1} = \dfrac{{{T_1}}}{{273.15K}}................( 5)

Cross multiply equation (5)
4×273.15=T1 T1=1092.6K \begin{gathered} 4 \times 273.15 = {T_1} \\\ {T_1} = 1092.6K \\\ \end{gathered}

Hence, The speed of sound will double at temperature of 1092.6K1092.6K

So, The correct option is C

Note: The speed of sound is variable and depends on the properties of the substance through which the wave is travelling. In solids, the speed of transverse waves depends on the shear deformation under shear stress, and the density of the medium. For air at sea level, the speed of sound is331m/s331m/s.